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OPA643 Datasheet(PDF) 8 Page - Texas Instruments |
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OPA643 Datasheet(HTML) 8 Page - Texas Instruments |
8 / 16 page 8 ® OPA686 APPLICATIONS INFORMATION WIDEBAND, NON-INVERTING OPERATION The OPA686 provides a unique combination of features— low input voltage noise along with a very low distortion output stage—to give one of the highest dynamic range op amps available. Its very high Gain Bandwidth Product (GBP) can be used either to deliver high signal bandwidths at high gains, or to deliver very low distortion signals at moderate frequencies and lower gains. To achieve the full perfor- mance of the OPA686, careful attention to PC board layout and component selection is required as discussed in the remaining sections of this data sheet. Figure 1 shows the non-inverting gain of +10 circuit used as the basis of the Electrical Specifications and most of the Typical Performance Curves. Most of the curves were char- acterized using signal sources with 50 Ω driving impedance, and with measurement equipment presenting a 50 Ω load impedance. In Figure 1, the 50 Ω shunt resistor at the V I terminal matches the source impedance of the test generator, while the 50 Ω series resistor at the V O terminal provides a matching resistor for the measurement equipment load. Generally, data sheet voltage swing specifications are at the output pin (VO in Figure 1), while output power (dBm) specifications are at the matched 50 Ω load. The total 100Ω load at the output, combined with the 503 Ω total feedback network load, presents the OPA686 with an effective output load of 83 Ω for the circuit of Figure 1. Voltage feedback op amps, unlike current feedback designs, can use a wide range of resistor values to set their gain. The circuit of Figure 1, and the specifications at other gains, use the constraint that RG should always be set to 50Ω and RF adjusted to get the desired gain. Using this guideline will guarantee that the noise added at the output due to Johnson noise of the resistors will not significantly increase the total noise over that due to the 1.3nV/ √Hz input voltage noise for the op amp itself. WIDEBAND, INVERTING GAIN OPERATION Operating the OPA686 as an inverting amplifier has several benefits and is particularly appropriate when a matched input impedance is required. Figure 2 shows the inverting gain circuit used as the basis of the inverting mode Typical Performance Curves. FIGURE 1. Non-Inverting, G = +10 Specification and Test Circuit. FIGURE 2. Inverting, G = –20 Characterization Circuit. Driving this circuit from a 50 Ω source, and constraining the gain resistor (RG) to equal 50Ω, will give both a signal bandwidth and noise advantage. RG acts as both the input termination resistor and the gain setting resistor for the circuit. Although the signal gain (VO/VI) for the circuit of Figure 2 is double that for Figure 1, the noise gains are in fact equal when the 50 Ω source resistor is included. This has the interesting effect of doubling the equivalent GBP of the amplifier. This can be seen in comparing the G = +10 and G = –20 small-signal frequency response curves. Both show approximately 250MHz bandwidth, but the inverting configuration of Figure 2 gives 6dB higher signal gain. If the signal source is actually the low impedance output of another amplifier, RG should be increased to the minimum load resistance value allowed for that amplifier and RF should be adjusted to achieve the desired gain. For stable operation of the OPA686, it is critical that this driving amplifier show a very low output impedance at frequencies beyond the expected closed-loop bandwidth for the OPA686. WIDEBAND, HIGH SENSITIVITY, TRANSIMPEDANCE DESIGN The high Gain Bandwidth Product (GBP) and the low input voltage and current noise for the OPA686 make it an ideal wideband transimpedance amplifier for low to moderate transimpedance gains. Very high transimpedance gains (> 100k Ω) will benefit from the low input noise current of a FET-input op amp such as the OPA655. Unity gain stability in the op amp is not required for application as a OPA686 +5V –5V –V S +V S 50 Ω V O V I 50 Ω + 0.1µF + 6.8µF 6.8µF R G 50 Ω R F 453 Ω 50 Ω Source 50 Ω Load 0.1µF OPA686 +5V –5V +V S –V S 91 Ω 50 Ω V O V I + 6.8µF 0.1µF + 6.8µF 0.1µF 0.1µF R F 1k Ω R G 50 Ω 50 Ω Source 50 Ω Load |
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